<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">OJAppS</journal-id><journal-title-group><journal-title>Open Journal of Applied Sciences</journal-title></journal-title-group><issn pub-type="epub">2165-3917</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojapps.2022.1212147</article-id><article-id pub-id-type="publisher-id">OJAppS-122135</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Biomedical&amp;Life Sciences</subject><subject> Chemistry&amp;Materials Science</subject><subject> Computer Science&amp;Communications</subject><subject> Engineering</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  &lt;i&gt;L&lt;/i&gt;&lt;sub&gt;1/2 &lt;/sub&gt;-Regularized Quantile Method for Sparse Phase Retrieval
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Si</surname><given-names>Shen</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Jiayao</surname><given-names>Xiang</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Huijuan</surname><given-names>Lv</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ailing</surname><given-names>Yan</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>School of Science, Hebei University of Technology, Tianjin, China</addr-line></aff><aff id="aff3"><addr-line>School of Insurance and Economics, University of International Business and Economics, Beijing, China</addr-line></aff><aff id="aff1"><addr-line>College of Science, Minzu University of China, Beijing, China</addr-line></aff><pub-date pub-type="epub"><day>08</day><month>12</month><year>2022</year></pub-date><volume>12</volume><issue>12</issue><fpage>2135</fpage><lpage>2151</lpage><history><date date-type="received"><day>16,</day>	<month>November</month>	<year>2022</year></date><date date-type="rev-recd"><day>27,</day>	<month>December</month>	<year>2022</year>	</date><date date-type="accepted"><day>30,</day>	<month>December</month>	<year>2022</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  The sparse phase retrieval aims to recover the sparse signal from quadratic measurements. However, the measurements are often affected by outliers and asymmetric distribution noise. This paper introduces a novel method 
  that
   combines the quantile regression and the L<sub>1/2</sub>-regularizer. It is a non-convex, non-smooth, non-Lipschitz optimization problem. We propose an efficient algorithm based on the Alternating Direction Methods of Multiplier (ADMM) to solve the corresponding optimization problem. Numerous numerical experiments show that this method can recover sparse signals with fewer measurements and is robust to dense bounded noise and Laplace noise.
 
</p></abstract><kwd-group><kwd>Sparse Phase Retrieval</kwd><kwd> Nonconvex Optimization</kwd><kwd> Alternating Direction Method of Multipliers</kwd><kwd> Quantile Regression Model</kwd><kwd> Robustness</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Phase retrieval is a problem in recovering the unknown signal x ∈ ℝ p from the following model:</p><p>y = | A x | 2 + ϵ (1)</p><p>where A = [ a 1 , a 2 , ⋯ , a n ] T ∈ ℝ n &#215; p is the known measurements matrix, n is the number of measurements, y = [ y 1 , y 2 , ⋯ , y n ] ∈ ℝ n is the squared-magnitude measurements, ϵ = [ ϵ 1 , ϵ 2 , ⋯ , ϵ n ] ∈ ℝ n is noise or outliers [<xref ref-type="bibr" rid="scirp.122135-ref1">1</xref>], |   ⋅   | 2 denotes the element-wise absolute-squared value. Especially, when both A and x belong to the real field, the problem is called real-valued phase retrieval [<xref ref-type="bibr" rid="scirp.122135-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.122135-ref3">3</xref>]. Phase retrieval problem has many important applications, including X-ray crystallography [<xref ref-type="bibr" rid="scirp.122135-ref4">4</xref>], optics [<xref ref-type="bibr" rid="scirp.122135-ref5">5</xref>], astronomy [<xref ref-type="bibr" rid="scirp.122135-ref6">6</xref>], and blind ptychography [<xref ref-type="bibr" rid="scirp.122135-ref7">7</xref>]. The methods to solve PR problems can be roughly divided into two categories: the first is based on alternating projection proposed by Gerchberg and Saxton. Examples include Hybrid Input-Output (HIO), Hybrid Projective Reflection, and so on. In recent years, some scientists have proposed more advanced alternating projection algorithms. The second is the convex method of semidefinite programming (SDP) or convex relaxation for quadratic equations in the dirt (1). The most representative is PhaseLift [<xref ref-type="bibr" rid="scirp.122135-ref8">8</xref>], which was proposed by Cand, Strohmer, and Voroninski. This is an algorithm for minimizing convex trajectories (kernels) using an SDP-enhanced technique. In many applications, especially those related to imaging, the signal x ∈ ℝ p allows sparse representation under certain known and deterministic linear transformations. Without losing generality, we assume that signal x itself is sparse in the rest of this paper. In this case, model (1) is called the sparse phase recovery model.</p><p>To solve the sparse problem, L p ( 0 &lt; p &lt; 1 ) norm regularization is a common approach in the field of compression perception. In further study of the phase diagram, [<xref ref-type="bibr" rid="scirp.122135-ref9">9</xref>] results are as follows: 1) As the p-value decreases, the solution obtained by L regularization becomes more sparse. 2) When 1 / 2 &lt; p &lt; 1 , L<sub>1/2</sub> regularization always gets the most sparse solution, and when 0 &lt; p &lt; 1 / 2 , there is no significant difference in L p regularization performance. Therefore, the L<sub>1/2</sub> regularization can be used as a representative of the L p ( 0 &lt; p &lt; 1 ) regularization.</p><p>For asymmetric noise or outliers, some stable results have been obtained. For example, [<xref ref-type="bibr" rid="scirp.122135-ref10">10</xref>] developed for minimizing the least squares empirical loss and designed a two stages algorithm, which starts with a weighted maximal correlation initialization and then follows by the reweighted gradient iterations. However, most of the above methods are built upon the least squares (LS) criterion which is optimal for Gaussian noise, but may not be optimal if the noise is not Gaussian or asymmetric. To enhance the robustness against asymmetric noise or outliers, introduced quantile regression (QR) method which includes LAD method as a special case. Compared to LAD method, QR method involves minimizing asymmetrically-weighted absolute residuals, which permits a much more accuracy portrayal of the relationship between the observed covariates and the response variables. Therefore, it is more approproate in certain non-Gaussian settings to use QR method. For these reasons, QR has attracted tremendous interest in the literature. Recently, the penalized QR method has also gained a lot of attention in the high dimensional linear models, see for example [<xref ref-type="bibr" rid="scirp.122135-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.122135-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.122135-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.122135-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.122135-ref15">15</xref>].</p><p>On the other hand, recall that L<sub>1/2</sub>-regularization introduced by [<xref ref-type="bibr" rid="scirp.122135-ref9">9</xref>] and [<xref ref-type="bibr" rid="scirp.122135-ref16">16</xref>] has been widely used in many fields since it can generate more sparse solutions under fewer measurements than L<sub>1</sub>-regularization. Inspired by these works, we here propose a novel method which consists of QR and an L<sub>1/2</sub>-regularization. We call this method L<sub>1/2</sub>-regularized quantile regression phase retrieval (L<sub>1/2</sub> QR PR). Because the L<sub>1/2</sub>-regularized problem is non-convex, non-smooth, non-lipschitz, it is difficult to solve directly. Therefore, we design an ADMM algorithm to solve the correspoding optmization. Fortunately, all subproblems have closed solutions and convergence is guaranteed. Numerical experiments show that the proposed method can recover sparse signals with fewer measurements and is robust to asymmetrically distributed noises such as dense bounded noises and Laplacian noises.</p><p>The rest of this article is organized as follows. In Section 2, we design a novel algorithm based on ADMM to solve our method L<sub>1/2</sub> QR PR and discuss the convergence of proposed algorithm. In Section 3, we use a large number of numerical experiments to prove the effectiveness and robustness of our algorithm. Conclusions and future work are presented in Section 4.</p></sec><sec id="s2"><title>2. Optimization Algorithm</title><sec id="s2_1"><title>2.1. The Problem Formulation</title><p>The optimization problem that we consider is minimizing the problem as follow:</p><p>min x ∈ R 1 n ∑ i = 1 n ρ τ ( 〈 a i , x 〉 2 − y i ) + λ ‖ x ‖ 1 / 2 1 / 2 , (2)</p><p>where</p><p>ρ τ ( t ) = { τ t ,       t ≥ 0 ( 1 − τ ) t , otherwise ,</p><p>x , y i , a i , n have been described in (1), τ ∈ ( 0,1 ) , 〈 ⋅ , ⋅ 〉 stands for the inner product. λ &gt; 0 is the regularized parameter, and ‖ x ‖ 1 / 2 1 / 2 = ∑ i = 1 p | x i | 1 / 2 .</p><p>Noting that lim ‖ x ‖ 2 → ∞ ‖ x ‖ 1 / 2 1 / 2 → ∞ and λ &gt; 0 , we obtain that</p><p>lim ‖ x ‖ 2 → ∞ 1 n ∑ i = 1 n     ρ τ ( ( a i T x ) 2 − y i ) + λ ‖ x ‖ 1 / 2 1 / 2 → ∞</p><p>which together with the continuity of the object function yields that Problem (2) has a bounded solution. To design an appropriate iterated algorithm, we give the following two lemmas.</p><p>Lemma 1. (see [<xref ref-type="bibr" rid="scirp.122135-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.122135-ref17">17</xref>]) The global solution t * of following problem has analytic expression,</p><p>arg   min t ∈ ℝ ( t − α ) 2 + μ | t | 1 / 2</p><p>t * = { f μ , 1 / 2 ( α ) , | α | &gt; 54 3 4 μ 2 / 3 0,     otherwise ,</p><p>where</p><p>α ∈ ℝ ,   f μ , 1 / 2 ( α ) = 2 3 α ( 1 + cos ( 2 π 3 − 2 3 φ μ ( α ) ) )</p><p>with</p><p>φ μ ( α ) = arccos ( μ 8 ( | α | 3 ) − 3 2 ) .</p><p>Lemma 2. The global solution h * of following problem has analytic expression,</p><p>h * = arg min h ∈ ℝ μ 2 ( h − α 1 ) 2 + ρ τ ( h 2 − α 2 ) ,</p><p>where α 1 , α 2 ∈ ℝ , μ &gt; 0 is a constant. It can be derived</p><p>h * = l μ ( α 1 , α 2 ) ,</p><p>where</p><p>l μ ( α 1 , α 2 ) = { α 1 1 + 2 τ μ , if   α 2 ≤ 0   or   α 2 &gt; 0   and   | α 1 | &gt; α 2 ( 1 + 2 τ μ ) α 2 , if   α 2 &gt; 0   and   0 ≤ α 1 ≤ α 2 ( 1 + 2 τ μ ) − α 2 , if   α 2 &gt; 0   and   − α 2 ( 1 + 2 τ μ ) ≤ α 1 ≤ 0 ,</p><p>0 &lt; μ ≤ 2 ( 1 − τ ) and</p><p>l μ ( α 1 , α 2 ) = { α 1 1 + 2 τ μ , if   α 2 ≤ 0   or   α 2 &gt; 0   and   | α 1 | &gt; α 2 ( 1 + 2 τ μ ) α 1 1 − 2 ( 1 − τ ) μ , if   α 2 &gt; 0   and   | α 1 | &lt; α 2 ( 1 − 2 ( 1 − τ ) μ ) α 2 , if   α 2 &gt; 0   and   α 2 ( 1 − 2 ( 1 − τ ) μ ) ≤ α 1 ≤ α 2 ( 1 + 2 τ μ ) − α 2 , if   α 2 &gt; 0   and   − α 2 ( 1 + 2 τ μ ) ≤ α 1 ≤ − α 2 ( 1 − 2 ( 1 − τ ) μ ) , (3)</p><p>as μ &gt; 2 ( 1 − τ ) .</p><p>One can get this lemma in the similar way of [<xref ref-type="bibr" rid="scirp.122135-ref18">18</xref>]. So, we omit the details.</p></sec><sec id="s2_2"><title>2.2. Solving the Objective with ADMM</title><p>We now employ the alternating direction method of multipliers (ADMM) algorithm to solve Problem (2). By introducing a pair of new variables, we reformulate Problem (2) as</p><p>min x , q , z 1 n ∑ j = 1 n ρ τ ( z i 2 − y i ) + λ ‖ q ‖ 1 / 2 1 / 2 s .t .       ( A I ) x − ( z q ) = 0, (4)</p><p>where z ∈ ℝ n and q ∈ ℝ p . Then, the augmented Lagrangian function of the above problem is</p><p>L r ( x , q , z ; Λ 1 , Λ 2 ) = 1 n ∑ i = 1 n     ρ τ ( z i − y i ) + λ ‖ q ‖ 1 / 2 1 / 2 + 〈 Λ 1 , x − q 〉     + r 2 ‖ x − q ‖ 2 2 + 〈 Λ 2 , A x − z 〉 + r 2 ‖ A x − z ‖ 2 2 , (5)</p><p>where Λ 1 , Λ 2 are the Lagrange multipliers, r is a positive constant.</p><p>Based on the framework of ADMM, the j + 1 th iteration can be calculated as</p><p>x j + 1 = arg min x L r ( x , q j , z j ; Λ 1 j , Λ 2 j ) , q j + 1 = arg min q L r ( x j + 1 , q , z j ; Λ 1 j , Λ 2 j ) , z j + 1 = arg min z L r ( x j + 1 , q j + 1 , z ; Λ 1 j , Λ 2 j ) , Λ 1 j + 1 = Λ 1 j + r ( x j + 1 − q j + 1 ) , Λ 2 j + 1 = Λ 2 j + r ( A x j + 1 − z j + 1 ) . (6)</p><p>In the following, we discuss the solution to each sub-minimization problem with respect to (w.r.t.) x , q , z .</p><p>1) Sub-minimization problem with respect to x: This problem can be written as</p><p>min x ∈ ℝ n 〈 Λ 1 j , x − q j 〉 + r 2 ‖ x − q j ‖ 2 2 + 〈 Λ 2 j , A x − z j 〉 + r 2 ‖ A x − z j ‖ 2 2 , (7)</p><p>Notice that</p><p>〈 Λ 1 j , x − q j 〉 + r 2 ‖ x − q j ‖ 2 2 + 〈 Λ 2 , A x − z j 〉 + r 2 ‖ A x − z j ‖ 2 2 = 〈 Λ 2 j , A x 〉 + 〈 Λ 1 j , x 〉 + r 2 ‖ A x − z j ‖ 2 2 + r 2 ‖ x − q j ‖ 2 2 . (8)</p><p>By the first order optimal condition, we can obtain the optimal solution. After analysis and comparison, we can conclude that</p><p>( r I + r A T A ) x j + 1 = r q j − A T Λ 2 j + r A T z j − Λ 1 j</p><p>where I stands for the identity matrix.</p><p>2) Sub-minimization problem with respect to q: This problem can be written as</p><p>min q ∈ ℝ n λ ‖ q ‖ 1 / 2 1 / 2 + 〈 Λ 1 j , x j + 1 − q 〉 + r 2 ‖ q − x j + 1 ‖ 2 2 . (9)</p><p>By simple calculation, one can see that the above problem is equivalent to the following minimization,</p><p>min q ∈ ℝ p λ ‖ q ‖ 1 / 2 1 / 2 + r 2 ‖ q − x j + 1 − Λ 1 j 2 ‖ 2 2 . (10)</p><p>According to the Lemma 1, we get</p><p>q d j + 1 = { f λ , 1 / 2 ( u d j ) , | u d j | &gt; 54 3 4 λ 2 / 3 0,     otherwise ,</p><p>where u d j = ( x j + 1 + Λ 1 j / 2 ) d is the d-th element of the vector x j + 1 + Λ 1 j / 2 , and d = 1,2, ⋯ , p .</p><p>3) Sub-minimization problem with respect to z: This problem can be written as</p><p>min z i ∈ ℝ , i = 1,2, ⋯ , n 1 n ∑ i = 1 n ρ τ ( z i 2 − y i ) + r 2 ‖ z − W j ‖ 2 2 . (11)</p><p>where W j = A x j + 1 + Λ 2 j / r . For each i = 1 , 2 , ⋯ , n , the following problem</p><p>min z i ∈ ℝ 1 n ρ τ ( z i 2 − y i ) + r 2 ( z i − W i j ) 2 (12)</p><p>can be solved by l n r ( 1, y i ( W i j ) 2 ) W i j based upon Lemma 2. To the ease of presentation, we introduce the notation L n r ( 1, y / | W | 2 ) ∈ ℝ n whose i-th element is defined as l n r ( 1, y i ( W i j ) 2 ) . Therefore, the problem (11) can be solved by</p><p>z j + 1 = L n r ( 1, y / | W j | 2 ) ⊙ W j ,</p><p>where ⊙ denote the Hadamard product, respectively.</p><p>According to the above analysis, the iterative scheme for solving (4) can be given in Algorithm 1.</p></sec><sec id="s2_3"><title>2.3. Convergence Analysis</title><p>As discussed above, one can see that each subproblem of the proposed algorithm is well defined. Therefore, we discuss its convergence. Consider q-sub-problem</p><disp-formula id="scirp.122135-formula4"><graphic  xlink:href="//html.scirp.org/file/12-2311867x66.png?20221229170505429"  xlink:type="simple"/></disp-formula><p>Algorithm 1. L<sub>1/2</sub>QR PR: ADMM method for solving (4).</p><p>min q ∈ ℝ n 1 2 ‖ q − u ‖ 2 2 + μ ‖ q ‖ 1 / 2 1 / 2 (16)</p><p>where μ &gt; 0 . According to [<xref ref-type="bibr" rid="scirp.122135-ref19">19</xref>], the first-order stationary point definition of (16) is given as follow.</p><p>Definition 1. Let q ^ be a vector in ℝ p and Q = Diag ( q ^ ) where Diag ( q ^ ) denotes a p &#215; p diagonal matrix whose diagonal is formed by the vector q ^ . The vector q ^ is a first-order stationary point of (16) if</p><p>Q ( q ^ − u ) + μ 2 | q ^ | 1 / 2 = 0.</p><p>Similar to [<xref ref-type="bibr" rid="scirp.122135-ref20">20</xref>], we introduce the Karush-Kuhn-Tucker (KKT) conditions of the Lagrangian L r ( x , q , z ; Λ 1 , Λ 2 ) in (2) as follows</p><p>{ ∂ x L r ( x ˜ , q ˜ , z ˜ , Λ ˜ 1 , Λ ˜ 2 ) = 0, r Q ˜ ( q ˜ − x ˜ + Λ ˜ 1 r ) + λ 2 | q ˜ | 1 / 2 = 0, ∂ z L r ( x ˜ , q ˜ , z ˜ , Λ ˜ 1 , Λ ˜ 2 ) = 0, ∂ Λ 1 L r ( x ˜ , q ˜ , z ˜ , Λ ˜ 1 , Λ ˜ 2 ) = 0, ∂ Λ 2 L r ( x ˜ , q ˜ , z ˜ , Λ ˜ 1 , Λ ˜ 2 ) = 0 (17)</p><p>where ( x ˜ , q ˜ , z ˜ , Λ ˜ 1 , Λ ˜ 2 ) is a saddle point, ∂ represents the partial derivative, q ˜ = Diag ( q ˜ ) , q ˜ is the first-order stationary point of q-subproblem (10).</p><p>Since the Lagrangian L r ( x , q , z ; Λ 1 , Λ 2 ) is nonconvex w.r.t. x , q , z . After analyzing the first-order optimality conditions for the variable z and the subproblem (12), the above KKT conditions corresponding to these three variables can be described as</p><p>A H Λ ˜ 2 + Λ ˜ 1 = 0,</p><p>Λ ˜ 2 | q ˜ | 2 − Q ˜ Λ ˜ 1 = 0,</p><p>( 2 n r s i g n ( | z ˜ m | 2 ) − y m ) z ˜ m − ( Λ ˜ 2 r + A x ˜ ) m ∋ 0, m = 1,2,3 , ⋯ , n ,</p><p>z ˜ = A x ˜ ,</p><p>x ˜ = q ˜ ,</p><p>where</p><p>s i g n ( x &#175; ) = { 1, x &#175; &gt; 0, − 1, x &#175; &lt; 0, 0, x &#175; &lt; 0.</p><p>Similar to Theorem 2.4 in [<xref ref-type="bibr" rid="scirp.122135-ref18">18</xref>], we show that our proposed algorithm converges to a saddle point satisfying KKT conditions.</p><p>Theorem 3. Assume that the successive differences of the two multipliers { Λ 1 j − Λ 1 j − 1 , Λ 2 j − Λ 2 j − 1 } converge to zero and { x j } is bounded. Then there exists a subsequence of iterative sequence of Algorithm 1 converging to an accumulation point that satisfies the KKT conditions of the saddle point problem (5).</p></sec></sec><sec id="s3"><title>3. Numerical Experiments</title><p>All simulations were performed on a 64-bit laptop computer running Windows 11 system with an AMD A8-6410 APU and 4 GB of RAM. To demonstrate the efficiency of our proposed method, we calculate the relative error between x o r i g and x ^ as</p><p>Relative   error : = min c = &#177; 1 ‖ x o r i g − x ^ ‖ 2 ‖ x o r i g ‖ 2 ,</p><p>where x o r i g is the true signal and x ^ is the solution obtained by a solver. In all experiments, we carry out 100 Monte Carlo runs.</p><sec id="s3_1"><title>3.1. Experimental Parameters and Initialization</title><p>We take p = 128 in all experiments, generating the true signal as Gaussian random sparse vector. The measurements matrix A generates from a i ∼ i . i . d . N ( 0, I ) . Regularization parameter λ is given by a fixed 10<sup>−4</sup>. The penalty parameter r is chosen as 10<sup>−2</sup>.</p><p>For nonconvex problems, ADMM can converge to different (and in particular, nonoptimal) points, depending on the initial values and the penalty parameter [<xref ref-type="bibr" rid="scirp.122135-ref21">21</xref>]. We take Wirtinger flow [<xref ref-type="bibr" rid="scirp.122135-ref22">22</xref>] with initial point q 0 , which obeys dist ( q 0 , x ) ≤ 1 8 ‖ x ‖ , where dist ( q , x ) = min c = &#177; 1 ‖ q − c x ‖ 2 . Hence the algorithm proposed converges from the neighborhood of the global minimizer.</p><p>Like many phase retrieval methods, we use spectral initial values to achieve better recovery. To evaluate the efficiency of our method, we compare the successful recovery rate with 5 kinds of algorithm listed in <xref ref-type="table" rid="table1">Table 1</xref>.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Comparison of reconstruction methods</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Method</th><th align="center" valign="middle" >Implementation</th><th align="center" valign="middle" >Measurements matrix</th><th align="center" valign="middle" >Robustness</th><th align="center" valign="middle" >Sparse solution</th></tr></thead><tr><td align="center" valign="middle" >L<sub>0</sub>L<sub>1</sub>PR [<xref ref-type="bibr" rid="scirp.122135-ref23">23</xref>]</td><td align="center" valign="middle" >ADMM</td><td align="center" valign="middle" >Fourier related</td><td align="center" valign="middle" >Noise</td><td align="center" valign="middle" >✓</td></tr><tr><td align="center" valign="middle" >LAD-ADMM [<xref ref-type="bibr" rid="scirp.122135-ref24">24</xref>]</td><td align="center" valign="middle" >ADMM</td><td align="center" valign="middle" >Gaussian</td><td align="center" valign="middle" >Gaussian mixture noises</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Median-RWF [<xref ref-type="bibr" rid="scirp.122135-ref1">1</xref>]</td><td align="center" valign="middle" >Gradient descent</td><td align="center" valign="middle" >Gaussian</td><td align="center" valign="middle" >Noise outliers</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >Median-MRWF [<xref ref-type="bibr" rid="scirp.122135-ref25">25</xref>]</td><td align="center" valign="middle" >Gradient descent</td><td align="center" valign="middle" >Gaussian</td><td align="center" valign="middle" >Noise outliers</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >L<sub>1/2</sub>LAD PR [<xref ref-type="bibr" rid="scirp.122135-ref18">18</xref>]</td><td align="center" valign="middle" >ADMM</td><td align="center" valign="middle" >Gaussian</td><td align="center" valign="middle" >Noise outliers</td><td align="center" valign="middle" >✓</td></tr><tr><td align="center" valign="middle" >L<sub>1/2</sub>QR PR</td><td align="center" valign="middle" >ADMM</td><td align="center" valign="middle" >Gaussian</td><td align="center" valign="middle" >Noise outliers</td><td align="center" valign="middle" >✓</td></tr></tbody></table></table-wrap></sec><sec id="s3_2"><title>3.2. Success Rate Comparisons</title><p>We compare the recovery success rates of L<sub>1/2</sub>QR PR at different values of τ in the noise-free case and noisy case including dense bounded noise and Laplace noise.</p><p>1) When not disturbed by noise, let τ = 0.1 , 0.2 , 0.4 , 0.5 , 0.6 , 0.8 , 0.9 . We report the success rates on <xref ref-type="table" rid="table2">Table 2</xref> where the recovery is considered successful if the relative error is less than 0.0001.</p><p>2) When in dense bounded noise, let τ = 0.1 , 0.2 , 0.4 , 0.5 , 0.6 , 0.8 , 0.9 . The entries of the dense bounded noise are generated independently from U ( 0 , η max ) , where η max / ‖ x ‖ 2 = 0.01 . We say that the recovery is successful if the relative error is less than 0.001. Since the recovery success rate is 0 as τ = 0.1 , we here report the other cases on <xref ref-type="table" rid="table3">Table 3</xref>.</p><p>3) When in Laplace noise, let τ = 0.4 , 0.5 , 0.6 , 0.8 , 0.9 and n / p = 4 , 5 , 6 . The entries of Laplace noise are generated from Laplace ( 0 , μ max / 2 ) , where μ max ‖ y ‖ 2 / n = 0.001 . We say that the recovery is successful if the relative error is less than 0.005 and report the success rate on <xref ref-type="table" rid="table4">Table 4</xref>.</p><p>From Tables 2-4, one can see that the recovery success rate of L<sub>1/2</sub>QR PR with τ = 0.5 is usually better than when τ equals other values. For Laplace noise, L<sub>1/2</sub>QR PR with τ = 0.5 and τ = 0.8 both perform well when n / p = 6 .</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Success rate of L<sub>1/2</sub>QR PR (Without noise)</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >τ</th><th align="center" valign="middle" >n/p = 2</th><th align="center" valign="middle" >n/p = 3</th><th align="center" valign="middle" >n/p = 4</th><th align="center" valign="middle" >n/p = 5</th><th align="center" valign="middle" >n/p = 6</th></tr></thead><tr><td align="center" valign="middle" >0.1</td><td align="center" valign="middle" >0.008</td><td align="center" valign="middle" >0.81</td><td align="center" valign="middle" >0.90</td><td align="center" valign="middle" >0.92</td><td align="center" valign="middle" >0.98</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.82</td><td align="center" valign="middle" >0.91</td><td align="center" valign="middle" >0.94</td><td align="center" valign="middle" >0.98</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.83</td><td align="center" valign="middle" >0.91</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle" >0.95</td></tr><tr><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >0.57</td><td align="center" valign="middle" >0.87</td><td align="center" valign="middle" >0.92</td><td align="center" valign="middle" >0.94</td><td align="center" valign="middle" >1.0</td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >0.46</td><td align="center" valign="middle" >0.86</td><td align="center" valign="middle" >0.90</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle" >0.99</td></tr><tr><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.56</td><td align="center" valign="middle" >0.85</td><td align="center" valign="middle" >0.89</td><td align="center" valign="middle" >0.93</td><td align="center" valign="middle" >0.96</td></tr><tr><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.55</td><td align="center" valign="middle" >0.84</td><td align="center" valign="middle" >0.88</td><td align="center" valign="middle" >0.92</td><td align="center" valign="middle" >0.97</td></tr></tbody></table></table-wrap><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Success rate of L<sub>1/2</sub>QR PR (Dense bounded noise)</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >τ</th><th align="center" valign="middle" >n/p = 4</th><th align="center" valign="middle" >n/p = 5</th><th align="center" valign="middle" >n/p = 6</th><th align="center" valign="middle" >n/p = 7</th><th align="center" valign="middle" >n/p = 8</th></tr></thead><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >0.65</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.70</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td></tr><tr><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.92</td><td align="center" valign="middle" >0.82</td><td align="center" valign="middle" >0.24</td><td align="center" valign="middle" >0.20</td></tr><tr><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.84</td><td align="center" valign="middle" >0.29</td></tr><tr><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.91</td><td align="center" valign="middle" >0.92</td><td align="center" valign="middle" >0.65</td><td align="center" valign="middle" >0.20</td></tr></tbody></table></table-wrap><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> Success rate of L<sub>1/2</sub>QR PR (Laplace noise)</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >τ</th><th align="center" valign="middle" >n/p = 4</th><th align="center" valign="middle" >n/p = 5</th><th align="center" valign="middle" >n/p = 6</th></tr></thead><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.22</td><td align="center" valign="middle" >0.40</td><td align="center" valign="middle" >0.73</td></tr><tr><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >0.49</td><td align="center" valign="middle" >0.88</td><td align="center" valign="middle" >0.96</td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >0.42</td><td align="center" valign="middle" >0.86</td><td align="center" valign="middle" >0.92</td></tr><tr><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.40</td><td align="center" valign="middle" >0.85</td><td align="center" valign="middle" >0.96</td></tr><tr><td align="center" valign="middle" >0.9</td><td align="center" valign="middle" >0.42</td><td align="center" valign="middle" >0.83</td><td align="center" valign="middle" >0.95</td></tr></tbody></table></table-wrap><p>Next, let’s continue to compare recovery success rate with the other five algorithms under different measurement fractions (n/p). We continue to use the same parameters and recovery success criteria as above. And let τ = 0.5 . <xref ref-type="fig" rid="fig1">Figure 1</xref> shows how these algorithms behave without noise. Through repeated experiments, we find that median-MRWF has a better recovery success rate when measurement fractions (n/p) = 2, 3 and no noise interference in real field. The recovery success rate of L<sub>1/2</sub>QR PR is slightly lower than that of median-RWF and median-MRWF, and higher than that of other algorithms. <xref ref-type="fig" rid="fig1">Figure 1</xref> also shows how these algorithms behave when disturbed by noise. When receiving interference from dense bounded noise, the recovery success rate of L<sub>1/2</sub>QR PR is higher than that of the other five algorithms in the real field. When receiving interference from laplace noise, the recovery success rate of L<sub>1/2</sub>QR PR is higher than that of the other five algorithms in the real field.</p><p>In the following chapters, we make τ = 0.5 . And we fix the sparsity to s = 8 and use the competing algorithms listed in L<sub>1/2</sub>QR PR the L<sub>1</sub> norm loss function, and L<sub>0</sub>L<sub>1</sub>PR adds L<sub>0</sub> regularization. The median-RWF and the median-MRAF of the L<sub>2</sub> norm loss function are highly robust to outliers through heuristic truncation rules. We compare the relative errors relative to the iteration count T under different measurement fractions (n/p), x is the true signal, x<sup> (t)</sup> is the tth iteration point.</p><p>Remark 3.1. We take n = 2p, 3p, 4p, 5p, 6p in real case. In detail, n = 2p and n = 4p are approximate theoretical sample complexity. When lad-admm returns to stability, we actually use n = 6p.</p></sec><sec id="s3_3"><title>3.3. Exact Recovery for Noise-Free Data</title><p>In the noise-free case, <xref ref-type="fig" rid="fig2">Figure 2</xref> shows in real case, when n = 2p, L<sub>1/2</sub>QR PR and L<sub>1/2</sub>LAD PR have good recovery performance. When n = 3p, 4p, 5p, 6p, L<sub>1/2</sub>QR PR is slightly better than other 5 algorithms.</p></sec><sec id="s3_4"><title>3.4. Stable Recovery with Dense Bounded Noise</title><p>Now, we consider the existence of dense bounded noise. The entries of the dense bounded noise are generated independently from U ( 0 , η max ) , where η max / ‖ x ‖ 2 = 0.001 , 0.01 . It can be seen from <xref ref-type="fig" rid="fig3">Figure 3</xref>, L<sub>1/2</sub>QR PR shows great robustness to dense bounded noise in real case, while LAD-ADMM shows poor performance. L<sub>1/2</sub>QR PR and L<sub>1/2</sub>LAD PR have similar performance when n = 4p</p><p>in real case. Median-RWF and median-MRAF have similar performance when n ≥ 4p in real case. Another reasonable observation, we find the relative reconstruction error has 10 times increase as η shrinks by a factor of 10 for all algorithms.</p></sec><sec id="s3_5"><title>3.5. Stable Recovery with Laplace Noise</title><p>Finally, we consider the presence of Laplace noise, the entries of Laplace noise are generated from Laplace ( 0 , μ max / 2 ) , where μ max ‖ y ‖ 2 / n = 0.001 , 0.01 . As can be observed in <xref ref-type="fig" rid="fig4">Figure 4</xref>, surprisingly, L<sub>1/2</sub>QR PR and L<sub>1/2</sub>LAD PR are very robust to Laplace noise, especially in real case, no matter when n = 2p, 3p, 4p, 5p, 6p. However, other methods show poor performance, even when n = 6p, LAD-ADMM, L<sub>0</sub>L<sub>1</sub>PR, median-RWF, median-MRAF don’t have satisfactory recovery. Another logical observation, we find the relative reconstruction error has 10 times increase as μ max shrinks by a factor of 10 for all algorithms.</p><p>The simulation results show that the L<sub>1/2</sub>QR PR algorithm with quantile loss function and L<sub>1/2</sub> regularization has two significant advantages over other methods. One is the ability to recover the signal with fewer measured values, and the other is the robustness to asymmetrically distributed noise (such as dense bounded noise and Laplacian noise).</p></sec></sec><sec id="s4"><title>4. Conclusion</title><p>We proposed the L<sub>1/2</sub> QR PR method and designed an efficient algorithm based on the framework of ADMM. A series of numerical experiments show that the proposed method can recover sparse signals with fewer measurements and is robust to asymmetrically distributed noises such as dense bounded noises and Laplace noises. An interesting future research direction is to consider the complex situations, such as Fourier basic measurements, which is an application of coded diffraction patterns [<xref ref-type="bibr" rid="scirp.122135-ref26">26</xref>].</p></sec><sec id="s5"><title>Acknowledgements</title><p>The authors would like to thank the editor and anonymous reviewers for their insight and helpful comments and suggestions which greatly improve the quality of the paper. The research was supported by the National Natural Science Foundation of China (NSFC) (11801130), the Natural Science Foundation of Hebei Province (A2019202135), the National Social Science Fund of China (17BSH140), “The Fundamental Research Funds for the Central Universities” in UIBE (16YB05) and “The Fundamental Research Funds for the Central Universities” (2022QNYL29).</p></sec><sec id="s6"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s7"><title>Cite this paper</title><p>Shen, S., Xiang, J.Y., Lv, H.J. and Yan, A.L. (2022) L<sub>1/2</sub>-Regularized Quantile Method for Sparse Phase Retrieval. 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